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Following Moroi in \cite{moroi} I see that for large $\tan\beta$
g-2 goes like 

\begin{eqnarray}
\delta a_\mu \propto \frac{m_\mu^2 \mu  \tan\beta}{M_{1/2}} J
\end{eqnarray}

where J is a loop factor depending on $\mu$ and $M_{1/2}$ 
slightly on $M_0$. For large $M_{1/2}$, $J\simeq 1/M_{1/2}$

Following Chankowski et.al and Urban et.al [my program]
the Wilson coefficients $c_{S,P}$ in 
${\cal B}(\bar{B}_s\rightarrow \mu^+ \mu^-)$ and for go like 

\begin{eqnarray}
|c_{S,P}| \propto  \frac{m_\mu m_t^2 \mu \tan\beta^3}{M_{1/2}} 
\end{eqnarray}



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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% 
\begin{thebibliography}{99}
\bibitem{moroi}
T.~Moroi,
%``The Muon Anomalous Magnetic Dipole Moment in the Minimal Supersymmetric Standard Model,''
Phys.\ Rev.\ D {\bf 53}, 6565 (1996)
[Erratum-ibid.\ D {\bf 56}, 4424 (1996)]
[hep-ph/9512396].
%%CITATION = HEP-PH 9512396;%%


\end{thebibliography}